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Table 1

Summary of parameters used to build up the fiducial simulation.

Gaseous disk Planetesimal disk
name Unit value name Unit value
Σ0 g cm–2 27.17 N 104
h0 0.05 amin au 75
rmin au 5 amax au 400
rmax au 400 e 0–0.01
r0 au 10 I degrees 0–0.60
P 0.5 ω degrees 0–360
Q 0.25 Ω degrees 0–360
Td Myr 2.75 f degrees 0–360
Td+$T_d^ + $ Myr 0.90
Planets
name Unit Planet e Planet d Planet c Planet b
mp Mjup 8.0 9.5 7.5 6.0
ainit au 15.12 24.22 39.86 65.49
alim au 30.24 48.44 79.72
e 0.163 0.131 0.052 0.009
I degrees 0.0 0.0 0.0 0.0
ω degrees 111.90 202.33 129.24 305.81
Ω degrees 0.0 0.0 0.0 0.0
f degrees 233.45 215.04 1.36 185.98
τa Myr 8.0
τa+$\tau _a^ + $ Myr 3.7 2.7 1.3
Γ˜${\tilde \Gamma }$ 0.75 0.75 0.75

Notes. Gaseous disk It has a surface density Σ0 and aspect ratio h0 at a reference radius of r0, and it extends from rmin to rmax. P and Q are the power-law indexes for the density and aspect-ratio profiles, respectively (Equations (10) and (11)). Td is the dispersal timescale of the gas disk, and Td+$T_d^ + $ is the acting timescale for the outward migration defined as one-third of Td. Planetesimal disk It is composed of N massless particles with each particle initialized with a semimajor axis a randomly such that they follow a power law ∝ a–0.5 from amin to amax. The rest of the orbital elements, inclination (I), argument of periapsis (ω), longitude of the ascending node (Ω), and true anomaly (f) are randomly chosen. Planets The planets have initial and fixed mass mp and initialized with a semimajor axis of ainit. The inward-migration timescale τα is defined for Planet b; meanwhile, the outward-migration timescale τa+$\tau _a^ + $ is defined for the rest. These outward-migrating planets have an upper limit for the semimajor axis alim and Γ˜${\tilde \Gamma }$ is the normalized torque.

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